Process for laser processing and apparatus for use in the same

ABSTRACT

A process for laser processing an article, which comprises: heating the intended article to be doped with an impurity to a temperature not higher than the melting point thereof, said article being made from a material selected from a semiconductor, a metal, an insulator, and a combination thereof; and irradiating a laser beam to the article in a reactive gas atmosphere containing said impurity, thereby allowing the impurity to physically or chemically diffuse into, combine with, or intrude into said article. The present invention also provides an apparatus for use in a laser processing process, characterized by that it is provided with an internal sample holder and a device which functions as a heating means of the sample, a window made of a material sufficiently transparent to transmit a laser beam, a chamber comprising a vacuum evacuation device and a device for introducing a reactive gas containing an impurity element, a laser apparatus operating in a pulsed mode to irradiate a laser beam to said chamber, and a means to move said chamber synchronously with the laser irradiation.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a technique which allows conducting adoping process or other chemical and physical treatments efficientlyeven at a low temperature.

2. Prior Art

Known processes for doping semiconductors with impurities include adiffusion process and an ion implantation process. The diffusion processcomprises heating the semiconductor to a high temperature in the rangeof from 1000 to 1200° C. to make the impurities diffuse intosemiconductors. In an ion implantation process, a predetermined portionof a semiconductor is bombarded with an ionized impurity which has beenaccelerated in an electric field.

The diffusion coefficient D of an impurity can be expressed with anexponential function of absolute temperature T as D=D₀·exp[−E_(a)/kT],where D₀ is the diffusion coefficient at T=∞, E_(a) is the activationenergy, and k is the Boltzmann constant. This equation describes theincrease of diffusion coefficient with elevating temperature;accordingly, it has been common practice to carry out diffusion attemperatures as high as possible, preferably, at 1000° C. or higher. Inthe ion implantation process, on the other hand, it is necessary toactivate the impurity and to remove the defects in the crystal latticedamaged by the ion bombardment; i.e., the implantation is followed byhigh-temperature annealing in the temperature range of from 600 to 950°C.

Recently, some types of active-matrix liquid crystal display devicesusing a thin-film transistor (TFT) provided on a glass substrate as theswitching device have brought into practical use. The source and drainregions in the TFTs of those display devices are, in general, formedmonolithically with the ohmic contacts using amorphous silicon havingeither of the N-type and P-type conductivity. Because the TFT used inthis case is of an inverse stagger type, it likely produces a parasiticcapacitance ascribed to its structure. To prevent this unwantedcapacitance from developing, there has been made studies on making useof a TFT having its source and drain being formed in a self-alignedstructure. However, the source and drain can be formed in a self-alignedmanner only by the use of an ion implantation or ion shower process.Then again, a post annealing at the temperature range of from 600 to950° C. should be carried out to activate the impurities and to recoverthe damage. Taking into consideration that the general purposeeconomical glass resists only up to a temperature of about 600 to 700°C., those ion implantation and ion shower processes are not feasible inan industrial operation.

As another means to circumvent the problem concerning the recover ofthermal damage on the glass substrates, there is known a technology,i.e., impurity doping using a laser beam irradiation. There is known,for example, a process which comprises first covering the intendedportion of the surface of the semiconductor with a thin film of theimpurity, and then irradiating a laser beam thereto to melt the thinfilm of the impurity simultaneously with the surface of thesemiconductor. In this manner, it is possible to dissolve the impurityinto the surface of the molten semiconductor.

In the process above using an excimer laser beam irradiation, theimpurity doping can be carried out without causing thermal damage on theglass substrate. However, the process requires an additional step ofcoating the semiconductor with the impurity. Conventionally, a coatingprocess such as spin coating has been used for this step. However, thequality of this coating is process-determining, because theconcentration of the doped impurity depends on the evenness of thiscoating. Thus, this process is far from being an ideal one. Furthermore,this coating is formed generally using an organic solvent as thesolution medium. The use of such an organic solvent sometimes allowsunfavorable elements such as carbon, oxygen, and nitrogen to enter intothe semiconductor to impair the properties thereof.

In the light of the circumstances described above, the present inventionhas been achieved with an aim to provide a laser-beam doping technologyusing particularly an excimer laser, said technology being composed ofsimplified process steps and free from invasion of foreign elements intothe semiconductor during the process. Accordingly, the present inventionprovides, with an object to simplify the process and to preventinclusion of undesirable elements, a doping process using a high puritydoping material in its gas phase in the place of the conventional solidor liquid phase doping materials. It is another object of the presentinvention to increase the doping efficiency.

Still other objects of the present invention include doping of elementsinto, in addition to semiconductors, various types of materialsinclusive of insulators and conductors, as well as modifying materialsand surfaces thereof. There can be specifically mentioned, for example,doping of phosphorus into a silicon oxide film.

SUMMARY OF THE INVENTION

The present invention provides an impurity doping process for impartingeither of the N-type and P-type conductivity to the samplesemiconductor, which comprises irradiating a laser beam to the surfaceof a semiconductor sample in a high purity reactive gas atmospherecontaining an impurity which renders the semiconductor N-conductive orP-conductive. It is known, however, based on the acquired knowledge ofthe present inventors, that the process at temperatures as low as theroom temperature is yet to be improved to achieve sufficient diffusionof the elements. In the process of the present invention, the laser beamis irradiated to the semiconductor with the semiconductor beingmaintained at a temperature higher than room temperature.

An embodiment according to the present invention provides, accordingly,a process which comprises heating the sample and maintaining it to atleast 200° C. during the irradiation of a laser beam, therebyaccelerating diffusion of the impurity elements and to dope thesemiconductor with the impurity at a high concentration. The temperatureto which the substrate is to be heated depend on the type of thesemiconductor, and is in the range of from 250 to 500° C., preferablyfrom 300 to 400° C., in the case of polysilicon (polycrystallinesilicon) and semi-amorphous silicon.

Thus heating the semiconductor is not only advantageous for thediffusion of the impurities, but also the semiconductor itself morereadily recovers the temporarily lost high crystallinity due to laserbeam irradiation, because heating the sample provides thermally asufficient relaxation time. A sample without being heated and subjectedto an irradiation of a laser beam, particularly to a beam of a laseroperating in a pulsed mode, experiences a typical rapid heating andrapid cooling. Hence, such samples are apt to turn into an amorphousstate. More specifically, the sample is instantaneously heated to atemperature as high as 1000° C. or even higher, but is then cooled toroom temperature during the next period of several hundreds ofnanoseconds. If we consider a case in which the sample is silicon and inwhich the sample is heated to the temperature range above, the timenecessary to reach the lower limit of the crystallization temperature,i.e., about 500° C., is calculated to be 10 times as long as thatnecessary to cool the sample to room temperature. If the duration oflaser beam irradiation exceeds a certain duration at this step, thesilicon melts to develop a convection which carries the impurities deepinto the internal of the silicon. On the other hand, if a pulsed laserbeam does not endure for a certain time, the silicon crystallizes into asolid to give a so-called semi-amorphous phase. In this case, theimpurities undergoes solid-phase diffusion to enter the internal of thesilicon.

It is unfavorable to heat the semiconductor to an excessively hightemperature. At too high a temperature, the reactive gas itselfundergoes pyrolysis (decomposition by heat) to form deposits not only onthe sample but also on the holder and the like. As a result, theefficiency of gas usage may be greatly impaired.

It is also undesirable to maintain the semiconductor at a temperaturehigher than the crystallization temperature thereof. This isparticularly so in the case of semiconductors comprising defects at highdensity, such as polycrystalline semiconductors, amorphoussemiconductors, and semi-amorphous semiconductors. If the doping were tobe taken place on a crystalline semiconductor being heated to atemperature of crystallization temperature or higher, the control forvalence electrons is almost lost due to the generation of energy levels.Accordingly, it is preferred that the process is conducted by heatingthe substrate at a temperature not higher than the temperature at whichamorphous silicon undergoes thermal transition to polysilicon, i.e.,from 500 to 550° C., and more preferably, at a temperature not higherthan a temperature lower than the transition temperature by 100° C.(i.e., about 400 to 450° C., or lower). In the case of a TFT usingamorphous silicon (referred to hereinafter as a-Si:TFT), the device isdestroyed if the temperature exceeds 350° C. Thus, such a-Si:TFTs shouldbe maintained at a temperature lower than 350° C. Such a care should betaken to other semiconductors as well.

Another embodiment according to the process of the present inventionprovides a technology for doping of an impurity from a gas phase using alaser, particularly an excimer laser, in which a plurality of elementsare doped using different types of doping gases. An object of thepresent process using a single laser beam is to avoid the drop in dopingefficiency due to the use of various doping gases differing in lightabsorption properties and in decomposition behavior. Accordingly, in thepresent process comprising irradiating a laser beam to the sample in areactive gas atmosphere containing an impurity which imparts either ofthe N- and P-conductive types to the semiconductor, an electromagneticenergy is applied to said reactive gas simultaneously with the laserirradiation to thereby decompose the reactive gas. The doping efficiencycan be further improved by heating the semiconductor to a pertinenttemperature in the same manner as in the first embodiment of the presentinvention. For example, this heating is carried out at a temperature nothigher than the crystallization temperature of the semiconductor underthe application of the electromagnetic energy.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows schematically the steps of a process for fabricating a TFTas described in the examples;

FIG. 2 shows schematically the steps of a process for fabricating a TFTas described in the examples;

FIG. 3 shows schematically the steps of a process for fabricating a TFTas described in the examples;

FIG. 4 shows schematically the steps of a process for fabricating a TFTas described in the examples;

FIG. 5 shows a schematically drawn apparatus used in Example 1, used forprocessing (impurity-doping) semiconductors;

FIG. 6 shows another schematically drawn apparatus used in Example 2,used for processing (impurity-doping) semiconductors;

FIG. 7 shows another schematically drawn apparatus used in Example 3,used for processing (impurity-doping) semiconductors;

FIG. 8 shows another schematically drawn apparatus used in Example 4,used for processing (impurity-doping) semiconductors;

FIG. 9 is a graph showing the distribution of impurity regions insemiconductors having fabricated by a conventional process and a processaccording to the present invention;

FIG. 10 shows schematically the steps of a process for fabricating a TFTas in Example 5;

FIG. 11 shows schematically the steps of a process for fabricating a TFTas in Examples 6 and 7;

FIG. 12 is a graph showing the C-V characteristics of a TFT havingfabricated in an Example;

FIG. 13 is a graph showing the distribution of an impurity (boron) alongthe thickness direction;

FIG. 14 is a graph showing the distribution of an impurity (phosphorus)along the thickness direction;

FIG. 15 is a graph in which the change in sheet resistance with varyingapplied energy density is plotted; and

FIG. 16 gives the characteristic curves for an inverter and a ringoscillator having fabricated by a process according to the presentinvention.

DETAILED DESCRIPTION OF THE INVENTION

In the process according to the present invention, the impurity whichimparts either of the N- and P-conductive types to the semiconductorrefers specifically to, in the case where a silicon semiconductor isused, a trivalent element, representatively boron (B) and the like, toimpart a P-type conductivity; and, a pentavalent impurity,representatively phosphorus (P), arsenic (As), etc., to impart an N-typeconductivity to the silicon semiconductor. Examples of the reactivegases containing those impurities include AsH₃, PH₃, BF₃, BCl₃, andB(CH₃)₃.

Most commonly used semiconductor for fabricating a TFT is a thin film ofan amorphous silicon semiconductor having deposited by a vapor phaseprocess, a sputtering process, etc. Also included are polycrystallineand single crystal silicon semiconductor films prepared from a liquidphase. Needless to say, semiconductors other than silicon can be used aswell.

A laser beam having generated from an excimer laser apparatus operatingin a pulsed mode is advantageously used. Laser beams in pulses ispreferred because the sample can be instantaneously heated, andmoreover, selectively heated only on the surface. This is advantageousbecause the substrate can be left intact. Because heating with a laseris confined to a small area of the sample, the use of a continuouslyoperating laser (such as argon ion laser) sometimes causes the heatedportion to fall off from the substrate due to considerable difference inthermal expansion coefficient between the substrate and the sample. Inusing a laser operating in a pulsed mode, however, this problem can beneglected because the thermal relaxation time is almost negligible ascompared with the reaction time of a mechanical stress such as thermalexpansion. Thus, the sample can be obtained without suffering anymechanical damage. Of course, there is little diffusion of impurities inthe substrate.

What is more advantageous is that the excimer lasers emit ultraviolet(UV) radiations. Because silicon and other semiconductors are goodabsorbers of UV light, those can efficiently absorb the beam. Theduration of a pulse is as short as 10 nsec. Furthermore, we can rely onan excimer laser considering the fact that it has been used inexperiments for obtaining thin films of polycrystalline silicon havinghigh crystallinity; the excimer laser has been irradiated on thin filmsof amorphous silicon for their crystallization. Specific examples ofsuitable excimer lasers include an ArF excimer laser (emitting light ofwavelength 193 nm), a XeC1 excimer laser (308 nm), a XeF excimer laser(351 nm), and a KrF excimer laser (248 nm).

In the process according to the present invention, the substrate isheated by using a conductive type holder in which a nichrome alloy wire,a kanthal alloy wire, or another heating element is directly assembled.Also useful are infrared-emitting lamps and any other of a radiationtype. However, the temperature of the substrate should be preciselycontrolled, because the concentration and the depth of the dopedimpurities are greatly influenced by the temperature of the substrate.Thus, the use of a temperature sensor such as a thermocouple isindispensable for the temperature control of the sample.

In the process according to the present invention, the reactive gas(referred to hereinafter as a “doping gas”) for use in doping ofimpurities is decomposed by applying thereto, in general, a 13.56-MHzhigh frequency wave energy as an electro-magnetic energy. The use ofthis auxiliary electromagnetic energy enables doping at a highefficiency even when a laser beam which by itself cannot directlydecompose the doping gas is used. The electromagnetic energy to use forthis purpose need not be only a high frequency wave of 13.56 MHz, andalso useful for obtaining a still higher activation ratio is, forexample, a microwave at a frequency of 2.45 GHz. Still further, therecan be taken advantage of an ECR (electron cyclotron resonance)condition which results from the mutual reaction between a 2.45-GHzmicrowave and a 875-Gauss magnetic field. It is also effective to use anoptical energy which is intense enough to directly decompose the dopinggas.

In the foregoing description, a technology for doping of impurities intoa semiconductor was referred. The present invention, however, can beapplied not only in the specified field above but also in a variety offields. For example, the present invention can be used in adding a traceelement to a metal for a mere several percent to a portion defined by acertain thickness from the surface, to thereby modify only the surfaceof the material. More specifically, nitrogen may be added to the surfaceof iron by conducting the process according to the present invention inammonia, to obtain a surface comprising iron nitride for a thickness offrom several to several hundreds of nanometers.

The present invention can be effectively applied to an oxide as well.For example, the process according to the present invention can becarried out on a thin film of a bismuth-based high temperature oxidesuperconductor in a lead chloride vapor, thereby adding lead into theoxide superconductor and hence elevate the critical temperature of thesuperconductor. Several types of bismuth-based oxide superconductors areknown to exist, but the highest achieved critical temperature to thepresent is about 110 K. However, it is difficult to obtain phases havinga critical temperature over 100 K. It is known also that the addition oflead into those superconductors readily provides phases with criticaltemperatures over 100 K, but in a practical process for fabricating thinfilms, lead tends to dissipate outside the oxide due to the heat fromthe substrate. In the process according to the present invention,however, the reaction takes place in disequilibrium. Hence, lead can beeffectively incorporated into the material having deposited into a thinfilm. Similarly, the process can be applied to a lead-containingferroelectric, PZT (lead zirconate titanate), which is now gaining muchattention as a functional material for semiconductor integratedcircuits, more particularly, for semiconductor memories.

The process according to the present invention can be used further foradding trace impurities into an insulator such as silicon oxide. Siliconoxide is frequently used as phosphosilicate glass (PSG) by addingseveral percent of phosphorus therein, as is customary in theconventional fabrication processes for semiconductors. Thus, phosphoruscan be added to silicon oxide using the process according to the presentinvention; for example, phosphorus may be added to silicon oxide anddiffused therein at a concentration of from 1×10²⁰ to 3×10²⁰ cm⁻³.

The phosphosilicate glass is known for its ability of preventing movableions such as sodium from invading the internal of the semiconductor. Ina conventional process, the phosphosilicate glass is deposited as a filmin an isolated CVD (chemical vapor deposition) chamber designedspecially for PSGs. The installation of such a CVD chamber requires anadditional cost. In contrast, the steps of doping of impurities anddepositing phosphosilicate glass can be performed in a single apparatusfor laser doping. Moreover, the film deposition apparatus for siliconoxide can be used widely in other applications. Accordingly, the totalcost can be reduced, and hence, it can be seen that the process iseconomical.

In particular, the process according to the present invention iseffective for improving film properties of the silicon oxide film havingdeposited at a relatively low substrate temperature of 600° C. or lower,using various types of organosilane compounds (e.g., tetraethoxysilane(TEOS)) as the starting material by vapor phase reaction. The processfor doping the silicon oxide film comprises irradiating a laser beam tothe surface of the silicon oxide film in a gas atmosphere containingphosphorus. In general, conventional films of this type containconsiderable amount of carbon which impair the insulating properties;moreover, those films had too many trap levels to be used as insulatorfilms for MOS structures and the like.

However, the film obtained by the process according to the presentinvention results in a considerably reduced amount of trap levels and inan improved insulating property. This is because carbon is driven awayfrom the film by the heat having generated by the laser irradiation. Asexplained hereinbefore, the distribution of the impurities along thedepth direction of the substrate can be controlled by changing thetemperature of the substrate. Accordingly, if a silicon oxide filmcontaining phosphorus deeply distributed therein is desired, thesubstrate is maintained at a temperature of 200° C. or higher, andpreferably, in the range of from 350 to 450° C. If a silicon oxide filmhaving phosphorus distributed within 100-nm depth or shallower, thesubstrate is maintained at a room temperature or lower.

If another semiconductor material such as amorphous silicon is providedunder the silicon oxide film at the laser doping, the crystallinitythereof is also improved at the same time by annealing. This occursbecause a silicon oxide film has low absorbance of UV light, and hence,the UV radiation having transmitted through the film is absorbed by thesemiconductor material lying underneath the silicon oxide film. Thissignifies that two steps can be put simultaneously in progress, and thatthe process according to the present invention is useful for enhancingmass-productivity.

In FIGS. 5 and 6 are shown schematically the apparatuses according tothe present invention. The apparatus illustrated in FIG. 5 is equippedonly with a substrate heating device (sample heating device), and thatin FIG. 6 comprises, in addition to the device above, an electromagneticdevice for generating a plasma. It should be noted that the figures areintended only for explanatory use, and in the practical operation ofthose apparatuses, they must be implemented with other parts ifnecessary. The mode of usage of those apparatuses is described below.

Referring to FIG. 5, explanation is made first on the apparatus showntherein. A sample 24 is mounted on a sample holder 25. First, a chamber21 is evacuated using an evacuation system 27 which is connected to anevacuation apparatus. This step is conducted because the atmosphericcomponents such as carbon, nitrogen and oxygen are least desirable forsemiconductors. Those elements are easily incorporated into thesemiconductor to sometimes lower the activity of the intentionally addedimpurities. Furthermore, they also impair the crystallinity of thesemiconductor and are causes of the formation of dangling bonds. Thus,the chamber is preferably evacuated first to a vacuum of 10⁻⁶ Torr orlower, and preferably, to 10⁻⁸ Torr or lower.

It is also favorable to drive out the atmospheric components havingadsorbed inside the chamber by operating a heater 26, together with,slightly before, or slightly after the evacuation. A structure, as iscommonly seen in a present-day vacuum apparatus, is preferred that apre-chamber is separately provided outside the chamber, because thechamber can be isolated from the atmosphere. As a matter of course, theuse of turbo molecular pumps and cryo-pumps which cause less carboncontamination and the like is preferred to rotary pumps andoil-diffusion pumps.

After once the chamber is sufficiently evacuated, a reactive gascontaining an impurity element is introduced into the chamber through agas system 28. The reactive gas may be a single component gas, or suchdiluted with hydrogen, argon, helium, neon, etc. It may be controlled toan atmospheric pressure or lower. These conditions are selected in viewof the type of the semiconductor to be processed, the concentration ofthe impurity, the depth of the impurity region, the temperature of thesubstrate, and the like.

Then, a laser beam 23 is irradiated through a window 22 from a laserdevice. At this instance, the sample is heated to a constant temperatureusing a heater. The laser beam is irradiated, in general, from about 5to 50 pulses per one site. Because the energy per pulse of the laserbeam considerably fluctuates, too few a repetition leads to theproduction of undesirable products at a high possibility. On the otherhand, too many a pulse repetition per site is also undesirable from theviewpoint of throughput. From the acquired knowledge of the presentinventors, a pulse repetition of from about 5 to 50 per site is optimalfrom the viewpoint of throughput and product yield.

In irradiating a laser beam having a particular shape, for example, a 10mm (along x direction)×30 mm (along y direction)-rectangle, the beam canbe irradiated in a pulse repetition of 10 times per site and then it canbe moved to the next site. Otherwise, the beam position can be moved 1mm each time along the x direction with the repetition of the pulse.

Upon completion of the laser irradiation step, the interior of thechamber is evacuated to vacuum, and the sample is taken out of thechamber after sufficiently cooling it to room temperature. It can beseen that the doping step is quite easily performed, and yet rapid. Thiscan be seen in clear contrast with a conventional ion implantationprocess which comprises three steps, i.e., (1) forming a doping pattern,which comprises coating the semiconductor with a resist, exposing, anddeveloping; (2) conducting ion implantation (or ion doping); and (3)recrystallizing the resulting semiconductor; or with a conventionalsolid phase diffusion process which comprises also three steps, i.e.,(1) forming a doping pattern, which comprises coating the semiconductorwith a resist, exposing, and developing; (2) coating the resultingstructure with an impurity film (by spin-coating, etc.); and (3)irradiating laser beam to the resulting structure. The process accordingto the present invention can be accomplished in two steps, i.e., (1)forming a doping pattern, which comprises coating the semiconductor witha resist, exposing, and developing; and (2) irradiating a laser beam tothe resulting structure.

A description similar to that given for the apparatus shown in FIG. 5can be applied to the one illustrated in FIG. 6. Firstly, a chamber 31is evacuated to vacuum through an evacuation system 37, and then areactive gas is introduced therein through a gas system 38. Then, alaser beam 33 is irradiated to a sample 34 having mounted on a sampleholder 35 through a window 32. At this instance, an electric power isapplied from a high frequency or an AC (or DC) power source 40 to anelectrode 39 to thereby generate a plasma and the like inside thechamber to activate the gas. The electrode in the figure is illustratedas a capacitance coupling type, but an inductance coupling type may beused in its place without any problem. Furthermore, even if acapacitance coupling type were to be used, the sample holder may be usedas the counter electrode. The sample may be heated with a heater 36during irradiating thereto a laser beam.

The present invention is described in further detail below referring tosome non-limiting examples.

EXAMPLE 1

An N-channel thin film gate-insulated field-effect transistor (referredto hereinafter as “NTFT”) established on a glass substrate wasfabricated according to a doping process of the present invention. Aglass substrate or a quartz substrate was used in this example. Suchsubstrates were selected because the TFTs thus fabricated were intendedfor switching devices and driving devices of an active matrix liquidcrystal display device or an image sensor. The process according to thepresent invention can be used as a doping technology in the fabricationof other semiconductor devices as well, such as the fabrication ofP-type and N-type semiconductor layers of a photoelectric conversiondevices, and the fabrication of single crystal semiconductor integratedcircuits (ICs). In such cases, single crystal and polycrystallinesubstrates of silicon and other semiconductors can be used as well asother insulators.

Referring to FIG. 1, the fabrication process is described. An SiO₂ filmor a silicon nitride film was first deposited on a glass substrate 11 togive a base protective film. In the present example, a 200 nm thick SiO₂film was deposited by RF sputtering in a 100% oxygen atmosphere underconditions as follows. Oxygen flow rate 50 sccm Pressure 0.5 Pa RF power500 W Substrate temperature 150° C.

Then, a 100 nm thick layer 13 of hydrogenated amorphous siliconsemiconductor, which is intrinsic semiconductor or substantiallyintrinsic (without artificially adding any impurity), was deposited onthe SiO₂ film by plasma-assisted CVD process. This layer 13 ofhydrogenated amorphous silicon semiconductor serves as a semiconductorlayer which provides a channel forming region and source and drainregions. The film deposition was conducted under conditions as follows.Atmosphere 100% silane (SiH₄) Film deposition temperature 160° C.(substrate temperature) Pressure at film deposition 0.05 Torr Inputpower 20 W (13.56 MHz)

In the present process, silane was used as the starting material fordepositing amorphous silicon. However, if the amorphous silicon is to bethermally crystallized into a polycrystalline silicon, disilane ortrisilane may be used as alternatives to silane to lower thecrystallization temperature.

The film deposition in this case was conducted in 100% silane instead ofcarrying out the process in a generally employed hydrogen-diluted silaneatmosphere. This was based on experimental results which showed that theamorphous silicon film having deposited in 100% silane can be moreeasily crystallized as compared with a one having deposited in ahydrogen-diluted silane. The film deposition was conducted at a lowtemperature in this case to incorporate a large amount of hydrogen intothe amorphous silicon film. In this manner, as many bondings as possiblecan be neutralized with hydrogen.

Furthermore, the input power of the high frequency wave energy (13.56MHz) in this example was as low as 20 W. By thus lowering the inputpower, the formation of silicon clusters, i.e., partially crystallineportion, during the film deposition can be avoided. This condition wasselected also based on the previous findings acquired throughexperiments. That is, the incorporation of a small crystalline portioninto the amorphous silicon film unfavorably affects the latercrystallization of the film which is conducted by irradiating a laserbeam.

Then, a patterning was carried out to separate the films into devices toobtain a structure as shown in FIG. 1. Subsequent to the patterning, thesample was heated in vacuum (of 10⁻⁶ Torr or lower) at 450° C. for anhour to thoroughly drive out hydrogen therefrom to form dangling bondsin high density.

The sample thus obtained was transferred into a laser irradiationapparatus as shown in FIG. 5, and was subjected to irradiation of anexcimer laser beam. In this manner the sample was crystallized intopolycrystalline silicon. In this step, a KrF excimer laser emitting alight at a wavelength of 248 nm was operated at a laser beam irradiatingenergy density of 350 mJ/cm² on a substrate heated to 400° C. The pulsedlaser beam was applied from 1 to 10 shots per site.

After the laser irradiation step, the sample was cooled to 100° C. in ahydrogen atmosphere under a reduced pressure of about 1 Torr.

In the present example, the crystallization of the amorphous siliconfilm was performed by irradiating a laser beam thereon. Alternatively, aheating process may be used for the crystallization of an amorphoussilicon semiconductor film provided on a glass substrate as well. Aheating process in this case comprises heating the sample at atemperature not higher than the heat-resistant temperature of the glass,specifically, in a temperature range of from 450 to 700° C. (in general,at 600° C.) for 6 to 96 hours.

In FIG. 5 is shown an apparatus comprising a vacuum chamber 21, a quartz(anhydrous quartz is preferred particularly in the case of excimerlaser) window 22 through which a laser beam is irradiated to the samplefrom the outside of the vacuum chamber 21, a laser beam 23 to irradiatethe sample, a sample 24, a sample holder 25, a heater 26 for heating thesample, an evacuation system 27, and an inlet system 28 for a gas of thestarting material, an inert gas, and a carrier gas. A practicalapparatus is generally equipped with a plurality of inlet systems, butin the figure is shown only one of those. In this example, a rotary pumpand a turbo-molecular pump were connected to the evacuation system toachieve a lower vacuum and a higher vacuum, respectively. Byappropriately using these two pumps, the concentration of the residualimpurities (particularly oxygen) was reduced to a level as low aspossible. The pumps to be used herein must be able to achieve a vacuumof 10⁻⁶ Torr or lower, and preferably, a vacuum of 10⁻⁸ Torr or lower.

After conducting the crystallization of the silicon film by operating anexcimer laser in a vacuum chamber, a 100 nm thick SiO₂ film 14 as a gateinsulator was deposited on the resulting structure by RF sputtering.Thus was obtained a structure shown in FIG. 2. Then, a 150 nm thickamorphous silicon semiconductor layer or polycrystalline siliconsemiconductor layer was deposited to give a gate electrode 15 on thegate insulating film 14. This layer was deposited incorporating P(phosphorus) to render the layer N-conductive. A structure as shown inFIG. 3 was thus obtained by patterning out a gate region. The gateelectrode may otherwise comprise a metal, such as aluminum, chromium,and tantalum. If aluminum or tantalum were to be used, the surfacethereof should be anodically oxidized to prevent the gate electrode fromsuffering damage at the later step of laser irradiation. For a planartype TFT comprising an anodically oxidized gate electrode, referenceshould be made to Japanese patent application Hei-3-237100 orHei-3-238713.

Then, to the structure as shown in FIG. 3, impurities were doped using alaser beam again in an apparatus shown in FIG. 5, in accordance with theprocess of the present invention. The sample placed inside the apparatusshown in FIG. 5 was heated under a PH₃ atmosphere, and a laser beam wasirradiated thereto to carry out doping of P (phosphorus). Accordingly,the source and drain regions (131 and 133 in FIG. 4) were renderedN-conductive because the source and drain regions were doped with theimpurity P (phosphorus). The channel-forming region (132 in FIG. 4),however, remained undoped because the gate insulator film 14 and thegate electrode 15 functioned as a mask to cut off laser beamirradiation. In FIG. 3, the channel region is located between the sourceand drain regions under the gate electrode in the semiconductor 13. Thedoping was carried out under conditions as follows. Atmosphere 5% PH₃(diluted with H₂) Sample temperature 350° C. Pressure 0.02-1.00 TorrLaser used KrF excimer laser (emitting light of 248 nm wavelength)Energy density 150-350 mJ/cm² Pulse repetition 10 shots

The source and drain regions can be activated simultaneously with thelaser doping.

After establishing the source and drain regions above, a 100 nm thickSiO₂ film 16 was deposited as an insulator film by RF sputtering asshown in FIG. 4. The film deposition conditions were the same as thoseemployed in the film deposition of the gate insulator.

In the next step, contact holes were provided by patterning, andfurther, aluminum was vapor deposited to establish a source electrode 17and a drain electrode 18. The resulting structure was thermally annealedat 350° C. in hydrogen to finish it into an NTFT. A P-channel TFT (a“PTFT”, hereinafter) could be fabricated similarly by using B₂H₆ in theplace of PH₃.

Furthermore, to assure the effect of the present invention, a sample wasprepared without heating it during irradiating a laser beam thereto, atthe same laser beam intensity as used in the process according to thepresent invention. The result is shown in FIG. 9(b). It can be seenclearly from these curves that the impurity concentration of a samplefabricated without heating the sample remained more than an order ofdegree lower, and the impurities were confined to the vicinity of thesurface. In contrast, the sample fabricated by heating it to 350° C.during the laser beam irradiation was found to contain the impurities ata high concentration and to have the impurities being diffused deep intothe sample as shown in FIG. 9(a).

As described in the foregoing, both an NTFT and a PTFT were fabricatedaccording to the process of the present invention. These TFTs werefurther assembled into a CMOS inverter, which was found to haveexcellent characteristics as shown in FIG. 16 (upper). Furthermore, aplurality of these CMOS circuits were assembled into a ring oscillator,which was also found to yield excellent characteristics as shown in FIG.16 (lower).

EXAMPLE 2

An NTFT established on a glass substrate was fabricated according to adoping process of the present invention. A glass substrate or a quartzsubstrate was used in this example as in Example 1. Then, an SiO₂ filmor a silicon nitride film was first deposited on a glass substrate 11 togive a base protective film 12 as shown in FIG. 1, following the sameprocess described in Example 1.

Then, a 100 nm thick layer 13 of hydrogenated amorphous siliconsemiconductor, which is intrinsic semiconductor or substantiallyintrinsic, was deposited on the SiO₂ film by plasma-assisted CVDprocess. A patterning process was then carried out to separate the filminto devices to obtain a structure as shown in FIG. 1. Subsequent to thepatterning, the sample was heated in vacuum (of 10⁻⁶ Torr or lower) at450° C. for an hour to thoroughly drive out hydrogen therefrom to formdangling bonds in high density.

In the same chamber in which the process of driving out hydrogen wasperformed, the sample thus obtained was subjected to irradiation of anexcimer laser beam while maintaining the vacuum. In this manner, thesample was crystallized into polycrystalline silicon under the sameconditions as those used in the process of Example 1. After the laserirradiation, the sample was cooled to 100° C. in a hydrogen atmosphereunder a reduced pressure of about 1 Torr.

In the present example, an apparatus as shown in FIG. 6 was usedthroughout the processes of heating the sample for removing hydrogen,crystallization of the sample by laser beam irradiation, and doping ofimpurities into the sample. Those processes were performed in the samesingle vacuum chamber. This is advantageous in that the sample can beeasily maintained in high vacuum throughout the processes and thatthereby the film can be maintained free from impurities (particularlyoxygen). The vacuum chamber can be used as a plasma-assisted CVDapparatus, as is equipped with an electrode for applying anelectromagnetic energy to the atmosphere. However, the processes abovemay be carried out separately in different reaction furnaces by using anapparatus having a multi-chamber arrangement. The reaction furnace inthis example had a positive column structure, but the structure of theuseful furnaces is not only limited thereto, and furnaces having othertypes of structures may be used as well. The manner of applying anelectromagnetic energy also is not particularly limited. An ECR typeapparatus may be used to achieve a further high activation ratio on thesamples.

In FIG. 6 is shown an apparatus comprising a vacuum chamber 31, a quartzwindow 32 through which a laser beam is irradiated to the sample fromthe outside of the vacuum chamber 31, a laser beam 33 to irradiate thesample, a sample 34, a sample holder 35, a heater 36 for heating thesample, an evacuation system 37, and an inlet system 38 for supplying agas of the starting material, an inert gas, and a carrier gas. Apractical apparatus is generally equipped with a plurality of inletsystems, but in the figure is shown only one of these. In this example,a rotary pump and a turbo-molecular pump were connected to theevacuation system to achieve a lower vacuum and a higher vacuum,respectively. An electromagnetic energy of 13.56 MHz which is generatedby a high frequency wave generator 40 is supplied to the chamber by apair of parallel planar electrodes 39.

After conducting the crystallization of the silicon film by operating anexcimer laser in a vacuum chamber as shown in FIG. 6, a 100 nm thickSiO₂ film 14 as a gate insulator was deposited on the resultingstructure by RF sputtering. Thus was obtained a structure shown in FIG.2. Then, a 150 nm thick amorphous silicon semiconductor layer orpolycrystalline silicon semiconductor layer was deposited to give a gateelectrode 15. This layer was deposited incorporating P (phosphorus) torender the layer N-conductive. A structure as shown in FIG. 3 was thusobtained by patterning out a gate region.

Then, to the structure as shown in FIG. 3, impurities were doped using alaser beam again in an apparatus shown in FIG. 6, in accordance with theprocess of the present invention. The sample placed inside the apparatusshown in FIG. 6 was heated under a PH₃ atmosphere being decomposed bythe applied electromagnetic energy, and a laser beam was irradiatedthereto to dope the sample with P (phosphorus). Accordingly, the sourceand drain regions (131 and 133 in FIG. 4) were rendered N-conductivebecause P was doped. The channel-forming region (132 in FIG. 4),however, remained undoped because the gate insulator film 14 and thegate electrode 15 functioned as a mask to cut off laser beamirradiation. The doping was carried out under conditions as follows.Atmosphere 5% PH₃ (diluted with H₂) Sample temperature 350° C. Pressure0.02-1.00 Torr Input energy 50-200 W Laser used KrF excimer laser(emitting light of 248 nm wavelength) Energy density 150-350 mJ/cm²Pulse repetition 10 shots

After establishing the source and drain regions above, a 100 nm thickSiO₂ film 16 was deposited as an insulator film by RF sputtering. Thefilm deposition conditions were the same as those employed in Example 1.In the next step, contact holes were provided by patterning, andfurther, aluminum was vapor deposited to establish a source electrode 17and a drain electrode 18. The resulting structure was thermally annealedat 350° C. in hydrogen to finish it into an NTFT.

A P-channel TFT (a “PTFT”, hereinafter) could be fabricated similarly bythis doping process, except for using B₂H₆ in the place of PH₃. Inconventional processes, the mixture of gases is decomposedheterogeneously upon irradiation of a laser beam at a single wavelengthdepending on the differing decomposition degree of each of the componentgases. The conventional processes thus suffered problematic non-uniformdoping. However, the process according to the present invention is freefrom being non-uniformly doped, because the doping gas in this processis decomposed not by the laser beam but by an additionally appliedelectromagnetic energy. Thus, uniform doping was achieved in both PTFTand NTFT without being influenced by the wavelength of the applied laserbeam.

EXAMPLE 3

In FIG. 7 is shown a doping apparatus according to the presentinvention, which comprises a chamber 71 provided with an anhydrousquartz slit window 72 through which a laser beam shaped into a thinrectangular form is irradiated to the sample. This laser beam is shaped,for example, into a rectangle 10 mm by 300 mm in size. The position ofthe laser beam is fixed. To the chamber are further connected anevacuation system 77 and an inlet system 78 for supplying the reactivegas. In the inside of the chamber are provided a sample holder 75 onwhich a sample 74 is mounted, and an infrared-emitting lamp 76 as aheater is set under the sample holder. The sample holder is movable sothat the sample may be moved in accordance with the laser shots.

An apparatus equipped with a mechanism for moving the sample thereinrequires much care in its temperature control, because the mechanism maysuffer mal-alignment due to dimensional change thereof caused by theheat generated by the heater. Furthermore, the chamber is a subject offrequent and troublesome maintenance work because the mechanism formoving the sample generates much dust.

EXAMPLE 4

In FIG. 8(A) is shown a doping apparatus according to the presentinvention, which comprises a chamber 81 provided with an anhydrousquartz window 82 sufficiently transparent to transmit a laser beam.Dissimilar to the window provided to the apparatus used in Example 3, itis a wide one which can cover the whole sample 84. To the chamber areconnected a vacuum evacuation system 87 and an inlet system 88 forsupplying the reactive gas (a gas containing an impurity element). Inthe inside of the chamber are provided a sample holder 85 on which asample 84 is mounted, and the sample holder is equipped with an internalheater which functions as a heating means of the sample. The sampleholder is fixed to the chamber. To the lower portion of the chamber isprovided a table 81 a for the chamber so that the whole chamber may bemoved in accordance with the laser shots. The laser beam used in thisExample was also shaped into a narrow rectangle as the one used inExample 3. For example, a laser beam shaped into a rectangle of 5 mm×100mm in size was used. Similarly again to the laser beam used in Example3, the position of the beam was fixed. The apparatus used in thisExample is different from that of Example 3 in that it employs amechanism to make the whole chamber movable. Thus, the inner of thechamber is free from those mechanical parts and hence generates no dust.By arranging the apparatus in this way, much effort for maintenance workcan be saved. Furthermore, the transport mechanism is independent of theheat generated from the heater.

The apparatus in the present Example is advantageous not only in thepoints mentioned hereinbefore, but also in the points as follows. Theapparatus used in Example 3 requires a long dead time, i.e., it took along time to get the laser fired after once a sample was loaded into thevacuum chamber, because a sufficient vacuum degree should be attained byevacuation. In the apparatus of the present Example, a plurality ofchambers (at least two chambers) as shown in FIG. 8(A) are provided sothat they may be rotated to perform sequentially the steps of chargingthe sample, evacuating the chamber to vacuum, irradiating a laser beamto the sample, and taking out the sample from the chamber. In thismanner, dead time can be completely eliminated from the process. In FIG.8(b) is shown a system employing the arrangement mentioned above.

In this system, chambers 96 and 97 charged with non-treated samples aretransferred during the evacuation step by a continuously movingtransportation mechanism 98 to a table 99 equipped with a precisionstage. The chamber 95 being mounted on the stage contains a sampletherein, and a laser beam having generated by a laser device 91operating in a pulsed mode and processed by pertinent optical devices 92and 93 is irradiated to the sample. After the sample is subjected to thedesired laser beam irradiation treatment by moving the stage and thechamber 95 synchronously with the laser irradiation, the chamber 94 istransferred to the next step again by a continuously movingtransportation mechanism 100. During this transportation step, theheater inside the chamber is turned off and the chamber is evacuated toget ready to take out the sample after it is sufficiently cooled.

As was described in the foregoing, the apparatus used in the presentExample cuts off the waiting time for being evacuated, and hence thethroughput can be increased. It should be noted, however, that thisprocess provides an increased throughput, but it requires many chambersto be installed. Hence, the apparatus must be chosen by taking intoconsideration the scale of mass production and of cost.

EXAMPLE 5

An NTFT established on a glass substrate was fabricated according to adoping process of the present invention. A glass substrate or a quartzsubstrate was used in this example as in Example 1. Then, an SiO₂ filmwas first deposited on a glass substrate 101 to give a base protectivefilm 102 as shown in FIG. 1, following the same process described inExample 1. Then, a 100 nm thick layer 103 of hydrogenated amorphoussilicon semiconductor, which is substantially intrinsic, was depositedon the SiO₂ film by plasma-assisted CVD process. A patterning processwas then carried out to separate the film into devices to obtain astructure as shown in FIG. 1. Subsequent to the patterning, the samplewas heated in vacuum (of 10⁻⁶ Torr or lower) at 450° C. for an hour tothoroughly drive out hydrogen therefrom to form dangling bonds in highdensity. A 100 nm thick SiO₂ film was then deposited on the resultingproduct by RF sputtering to obtain a structure shown in FIG. 10(A). Asilicon oxide mask 105 was left over only on channel portions.

Then, an impurity was doped in the sample according to a process of thepresent invention using a laser beam in an apparatus as shown in FIG. 6.The sample as shown in FIG. 10(B) was placed in the apparatus, and washeated under PH₃ atmosphere having decomposed by the appliedelectromagnetic energy. To the sample was then irradiated a laser beamto carry out the doping of P (phosphorus). Accordingly, the source anddrain regions (106 and 108 in FIG. 10(B)) were rendered N-conductivebecause P was doped. The channel-forming region (107 in the samefigure), however, remained undoped because the silicon oxide mask 105functions to cut off laser beam irradiation. Accordingly, thischannel-forming region was crystallized but remained undoped. It can beseen that a crystallization step and a doping step using a laser beamwas conducted at the same time. The doping was carried out under thesame conditions as those used in Example 2.

After establishing the source and drain regions above, a gate oxide film110 and a gate electrode 109 were deposited, and a 100 nm thick SiO₂film 111 was further deposited thereon as an interlayer insulator.Further thereafter, contact holes were patterned, and aluminum was vapordeposited thereon to give a source electrode 112 and a drain electrode113. Thus was the structure finished into an NTFT as shown in FIG. 10(C)by thermally annealing it in hydrogen at 350° C.

In the process described in the present Example, source and drain cannotbe formed in a self-aligned manner. However, the crystallization of thechannel region and the doping of the source and drain can be performedsimultaneously as in the process of the present Example by, forinstance, establishing first a gate electrode on the gate insulator filmin the similar manner as in Example 1 and then irradiating a laser beamfrom the back of the gate insulator film.

EXAMPLE 6

An active matrix as shown in FIG. 11 was fabricated on a Coning 7059glass substrate. The substrate 201 was a 1.1 mm thick Coning 7059 glass300×400 mm×1.1 mm in size as shown in FIG. 11(A). The substrate wascoated with silicon nitride film 202 by plasma-assisted CVD to athickness of from 5 to 50 nm, preferably, from 5 to 20 nm, so as toprevent the impurities such as sodium initially present in the substratefrom being diffused into the TFT. For technologies forming a blockinglayer by coating the substrate with silicon nitride or aluminum oxide,reference should be made to Japanese patent application Hei-3-238710 orHei-3-238714, filed by the present inventors.

After then depositing a silicon oxide film as a base oxide film 203, asilicon film 204 was deposited by a low-pressure CVD or plasma-assistedCVD process to a thickness of from 30 to 150 nm, preferably from 30 to50 nm. A silicon oxide film was deposited further thereon as a gateinsulator film 205 using tetraethoxysilane (TEOS) as the startingmaterial, by a plasma-assisted CVD process in oxygen atmosphere to athickness of from 70 to 120 nm, typically, to a thickness of 100 nm. Thesubstrate was maintained throughout to a temperature of 400° C. orlower, preferably, in the temperature range of from 200 to 350° C. toprevent shrinking or warping from occurring on the glass substrate.However, in this temperature level, the oxide film suffered formation ofa large number of recombination centers therein to give, for example, aninterface level density of 10¹² cm⁻² or higher. Thus, it was foundunfeasible to use the oxide film as a gate insulator.

Accordingly, the structure was subjected to a KrF laser irradiation in ahydrogen-diluted phosphine (5% PH₃) atmosphere as shown in FIG. 11(A) tohave the crystallinity of the silicon film 204 improved and also to havethe quantity of the recombination centers (trap centers) of the gateoxide film 205 reduced. The laser was operated at a beam energy densityof from 200 to 300 mJ/cm², and at a pulse repetition of 10 shots.Preferably, the temperature is maintained in the range of from 200 to400° C., representatively, at 300° C. As a result, the silicon film 204was improved in crystallinity, and the gate oxide film 205 was found tocontain doped phosphorus at a density of from 1×10²⁰ to 3×10²⁰ cm⁻³ andto have a reduced interface level density of 10¹¹ cm⁻² or lower.

Then, an aluminum gate electrode 206 was deposited on the resultingproduct to give a structure as shown in FIG. 11(B), and the peripherythereof was further coated with an anodically oxidized product 207.

Then, boron, an impurity for imparting P-conductivity, was implanted ina self-aligned manner into the silicon layer by an ion doping process togive a source and a drain 208 and 209 of the TFT, followed by theirradiation of a KrF laser to recover for the damage given to thesilicon film during the ion doping. For this purpose, the laser beam wasirradiated at a relatively high energy density of from 250 to 300mJ/cm². The resulting source and drain yielded a sheet resistance offrom 300 to 800 Ω/cm².

As shown in FIG. 11(D), an interlayer insulator 210 was provided usingpolyimide, and a pixel electrode 211 was established thereon using ITO(indium-tin-oxide). Furthermore, as shown in FIG. 11(E), contact holeswere bore to provide chromium electrodes 212 and 213 on the source anddrain regions of the TFT. One of the electrodes, the electrode 213, wasfurther connected to the ITO electrode. Thus, the structure was finishedinto a pixel for a liquid crystal display device by annealing theresulting product in hydrogen at 300° C. for 2 hours.

EXAMPLE 7

A TFT was fabricated by doping of phosphorus into a silicon oxide filmto give a gate insulator film as in Example 6. Similar to the processemployed in Example 6, a silicon nitride film 202 was deposited over thewhole surface of a substrate 201 by plasma-assisted CVD, to a thicknessof from 5 to 50 nm, preferably, from 5 to 20 nm. Then, after depositinga silicon oxide film as the base oxide film 203, a silicon film 204 wasdeposited by a low-pressure CVD or plasma-assisted CVD process to athickness of from 30 to 150 nm, preferably from 30 to 50 nm. A siliconoxide film was deposited further thereon as a gate insulator film 205 bysputtering to a thickness of from 70 to 120 nm, typically, to athickness of 100 nm. Alternatively, this step may be performed usingtetraethoxysilane (TEOS) as the starting material, by a plasma-assistedCVD process in oxygen atmosphere as in Example 6. The substrate wasmaintained throughout to a temperature of 400° C. or lower, preferably,in the temperature range of from 200 to 350° C. to prevent shrinking orwarping from occurring on the glass substrate.

Then, the structure was subjected to a KrF laser irradiation in ahydrogen-diluted phosphine (5% PH₃) atmosphere as shown in FIG. 11(A) tohave the crystallinity of the silicon film 204 improved and also to havethe quantity of the recombination centers (trap centers) of the gateoxide film 205 reduced. The laser was operated at a beam energy densityof from 200 to 300 mJ/cm², and at a pulse repetition of 10 shots. Thesubstrate was maintained at room temperature during the process.Accordingly, the doped phosphorus was confined within a region at adepth from the surface of 70% or less of the total thickness of thelayer.

An aluminum gate electrode 206 was then deposited on the resultingproduct to give a structure as shown in FIG. 11(B), and the peripherythereof was further coated with an oxide 207 obtained by anodicoxidation. Upon completion of the anodic oxidation, a negative voltagewas inversely applied to the resulting product. More specifically, avoltage in the range of from −100 to −200V was applied for a duration offrom 0.1 to 5 hours. The substrate was maintained in the temperaturerange of, preferably, from 100 to 250° C., and representatively, at 150°C. By carrying out this process, the movable ions which were present insilicon oxide or in the interface between silicon oxide and silicon wereattracted to the gate electrode A1, and were trapped in the midway bythe region containing phosphorus at a high concentration. Assumably,these phosphorus-rich regions are present as phosphosilicate glass. Fordetails on this technique comprising applying a negative voltage to thegate electrode during or after the anodic oxidation process, referenceshould be made to Hei-4-115503, filed by the present inventors on Apr.7, 1992.

Then, phosphorus, an impurity for imparting N-conductivity, wasimplanted in a self-aligned manner into the silicon layer by a known iondoping process to give a source and a drain 208 and 209 of the TFT,followed by the irradiation of a KrF laser as in FIG. 11(C), to recoverfor the damage given to the silicon film during the ion doping. As shownin FIG. 11(D), an interlayer insulator 210 was provided using polyimide,and a pixel electrode 211 was established thereon using ITO(indium-tin-oxide). Furthermore, as shown in FIG. 11(E), contact holeswere bore to provide chromium electrodes 212 and 213 on the source anddrain regions of the TFT. One of the electrodes, the electrode 213, wasfurther connected to the ITO electrode. Finally, a TFT was obtainedafter annealing the resulting product in hydrogen at 300° C. for 2hours.

EXAMPLE 8

A MOS (metal-oxide semiconductor) capacitor was fabricated by using agate oxide film having prepared by laser doping a silicon oxide film ona single crystal substrate with phosphorus. The C-V characteristic curveof this MOS capacitor was obtained.

A silicon oxide film was deposited as a gate insulator film on a (100)plane of single crystal silicon, to a thickness of from 70 to 120 nm,typically to a thickness of 100 nm, by plasma-assisted CVD usingtetraethoxysilane (TEOS) as a starting material in an oxygen atmosphere.The substrate was maintained at a temperature of 400° C. or lower,preferably, in the temperature range of from 200 to 350° C. However, inthis temperature level, the oxide film was found to contain a largenumber of clusters containing carbon, and it also suffered formation ofa considerable number of recombination centers to give, for example, aninterface level density of 10¹² cm⁻² or higher. Thus, it was foundunfeasible to use the oxide film as a gate insulator.

Accordingly, the structure was subjected to a KrF laser irradiation in ahydrogen-diluted phosphine (5% PH₃) atmosphere in the same apparatus asused in FIG. 1 to have the quantity of the recombination centers (trapcenters) of the silicon oxide film reduced. The laser was operated at abeam energy density of from 200 to 300 mJ/cm², and at a pulse repetitionof 10 shots. Preferably, the temperature is maintained in the range offrom 200 to 400° C., representatively, at 300° C. As a result, the oxidefilm was found to contain doped phosphorus at a density of from 1×10²⁰to 3×10²⁰ cm⁻³ and to have a reduced interface level density of 10¹¹cm⁻² or lower. Then, an aluminum gate electrode was deposited thereon.

A MOS capacitor fabricated without performing the laser, doping processyields, for example, a C-V curve having a large hysteresis as shown inFIG. 12(A). In the figure, the abscissa is the voltage and the ordinateis the electrostatic capacity. A MOS capacitor subjected to a laserdoping treatment according to the present invention yields a favorableC-V curve as shown in FIG. 12(B), which is in sharp contrast with theC-V curve of FIG. 12(A).

The film thus obtained by the process according to the present inventioncontains each of the elements distributed in the film in a manner asshown in FIG. 12(C). It can be seen that the silicon oxide film havingsubjected to laser doping according to the present invention is dopedwith phosphorus to about a half of the total depth of the film, and thatgettering was effected on sodium atoms thereby. It can be seen also thatlittle or no carbon is present over the whole oxide film. This isbecause carbon was driven out from the film by laser irradiation. It isfurther effective to apply a negative voltage to the aluminum gateelectrode as in Example 7, because the movable ions such as sodium ionspresent in the film can be attracted to the phosphorus-rich regions.

EXAMPLE 9

A 500 nm thick amorphous silicon film provided on a glass substrate wasdoped with an impurity by a process according to the present invention,and the film characteristics thereof were obtained. The results aregiven in FIGS. 13 to 15. The laser used in this Example was a KrF laseremitting a beam at a wavelength of 248 nm. The chamber used in thepresent process was like the one shown in FIG. 5. It was attempted inthis Example to change the doped impurity by introducing different typesof gases into the chamber. More specifically, a hydrogen gas containing5% phosphine was supplied to the chamber during the laser irradiation toadd an impurity which imparts N-conductivity to the semiconductor, and ahydrogen gas containing 5% diborane was introduced to the chamber duringthe laser irradiation to render the semiconductor P-conductive by dopingof the impurity.

The chamber was maintained at a pressure of 100 Pa. The laser wasirradiated at an energy density of from 190 to 340 mJ/cm², and the pulsewas provided at a repetition of from 1 to 100 shots. The temperature ofthe substrate was maintained at room temperature (R.T.) or at 300° C.

In FIGS. 13 and 14 are shown the change in diffusion of the impuritieswith varying substrate temperatures. In this case, the laser wasoperated at an energy density of 300 mJ/cm² and at a pulse repetition of50 shots. FIG. 13 was obtained from the data collected by secondary ionmass spectroscopy (SIMS), and it shows how boron diffuses along thedepth direction. As is clearly read from this figure, the impurityconcentration was an order of magnitude higher for the sample providedat a substrate temperature of 300° C., as compared with that of a samplemaintained at a substrate temperature of R.T.; also, the diffusion depthfor the former was about twice as large as that of the latter.

In FIG. 14 is shown the distribution of phosphorus along the depthdirection of the sample. A similar tendency as in the case of thedistribution of boron was observed. The effect of heating the substratewas particularly prominent in the case of adding phosphorus.

In FIG. 15 are plotted the sheet resistances with varying laser energydensity and number of shots. Boron was doped as the impurity. As thefigure clearly reads, the sheet resistance decreases and the impurityconcentration increases with increasing energy density. However, thesheet resistance seems to converge on a constant value.

Furthermore, despite the sheet resistance was observed to decrease withincreasing number of shots, no considerable decrease in sheet resistancewas observed at a laser, energy density of 220 mJ/cm² or higher in bothcases of 50 shots and 100 shots. However, there was observed a greatdifference between the sheet resistances obtained for 1 shot and 5shots. Accordingly, it was confirmed that the laser pulses at least 5shots are necessary to achieve a stable laser irradiation.

As described in the foregoing, a semiconductor can be efficiently dopedwith an impurity which imparts either an N-conductivity orP-conductivity to the doped product by the process according to thepresent invention, said process comprising irradiating a laser beam tothe semiconductor in an atmosphere containing the impurity above whileheating the sample or while applying an electromagnetic energy to areactive gas to decompose it into an atmosphere containing the impurityabove. In particular, the process according to the present invention iseffective in that the doping can be conducted without damaging the glasssubstrate, yet without being influenced by the wavelength of the laserused and by the type of the doping gas used in the process.

Furthermore, as mentioned earlier, the present invention is industriallyvaluable because it not only is confined to the field of dopingsemiconductors with impurities, but also is applicable to a variety offields, such as the surface modification of metal and ceramic materialsand the addition of trace elements into thin films of metal, ceramics,and insulators.

While the invention has been described in detail and with reference tospecific embodiments thereof, it will be apparent to one skilled in theart that various changes and modifications can be made therein withoutdeparting from the spirit and scope thereof.

1. A method of manufacturing a semiconductor device comprising steps of:irradiating a linear laser beam to a surface of a semiconductor in a gasatmosphere containing an impurity while scanning the linear laser beam;and applying an electromagnetic energy to the gas atmosphere so as todecompose the gas containing the impurity while irradiating the linearlaser beam.